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Rotational power in rotational motion is...

Rotational power in rotational motion is -

A

`vecomega.vectau`

B

`vecomegaxxvectau`

C

`omegaxxtau`

D

`tauxxomega`

Text Solution

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The correct Answer is:
To find the rotational power in rotational motion, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Definition of Power**: Power is defined as the rate at which work is done. In the context of rotational motion, we need to relate this to torque and angular displacement. 2. **Relate Work Done to Torque**: The work done (W) in rotational motion can be expressed as: \[ W = \tau \cdot d\theta \] where \( \tau \) is the torque and \( d\theta \) is the small angular displacement. 3. **Find the Rate of Work Done**: To find the power (P), we take the derivative of work with respect to time (t): \[ P = \frac{dW}{dt} = \frac{d(\tau \cdot d\theta)}{dt} \] 4. **Use the Chain Rule**: By applying the chain rule, we can express this as: \[ P = \tau \cdot \frac{d\theta}{dt} \] Here, \( \frac{d\theta}{dt} \) is the angular velocity (\( \omega \)). 5. **Express Power in Terms of Torque and Angular Velocity**: Substituting \( \omega \) into the equation gives us: \[ P = \tau \cdot \omega \] This equation represents the instantaneous power in rotational motion. 6. **Consider the Direction of Vectors**: If the torque and angular velocity are not in the same direction, we can express the power as the dot product: \[ P = \tau \cdot \omega \] This indicates that the power is the component of torque in the direction of angular velocity. ### Final Result: The rotational power in rotational motion is given by: \[ P = \tau \cdot \omega \]
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Knowledge Check

  • A couple produces: a) purely translational motion b) purely rotational motion c) both translational and rotational motion d) no motion

    A
    purely translational motion
    B
    purely rotational motion
    C
    both translational and rotational motion
    D
    no motion
  • Analogue of mass in rotational motion is.

    A
    moment of inertia
    B
    torque
    C
    radius of gyration
    D
    angular momentum
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    The moment of inertia in rotational motion is equivalent to :

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    Assertion : In rotational plus translational motion of a rigid body, different particles of the rigid body may have different velocities but they will have same accelerations Reason : Translational motion of a particle is equivalent to the translation motion of a rigid body.

    Can we use the equations of rotational motion if theta is measured in degrees and not in radian ?

    (A) : Moment of inertia plays the same role in rotational motion, as mass plays in linear motion. (R ) : Moment of inertia depends only on mass of the body.